Seesion1 summary Unwanted Beam Workshop (UBW 2012) 17.-18.12 2012 Dark Current Issues for Energy Recovery Linacs.

Slides:



Advertisements
Similar presentations
The JLab IR/UV FEL Driver D. Douglas for the JLab FEL anarcho-syndicalist commune.
Advertisements

Slide 1 Light Source Research at Jefferson Lab George R. Neil and Gwyn P. Williams Associate Director, Jefferson Laboratory JSA Science Council January.
Tom Powers Practical Aspects of SRF Cavity Testing and Operations SRF Workshop 2011 Tutorial Session.
Compton polarimetry for EIC Jefferson Lab Compton Polarimeters.
Halo, SLAC, 2014 Towards wire scanner measurements with Large Dynamic Range (> 10 6 ) Pavel Evtushenko, Jefferson Lab.
Chris Tennant Jefferson Laboratory March 15, 2013 “Workshop to Explore Physics Opportunities with Intense, Polarized Electron Beams up to 300 MeV”
11/05/09 Slide 1 Workshop Summary: Accelerator Physics for Future Light Sources William A. Barletta Director, United States Particle Accelerator School.
Recirculating pass optics V.Ptitsyn, D.Trbojevic, N.Tsoupas.
ERHIC Main Linac Design E. Pozdeyev + eRHIC team BNL.
1 Low-energy RHIC electron Cooler (LEReC) Update November 17, 2014.
Aperture Considerations in the FEL Upgrade Accepted design process –generate design  known –set aperture = N  + W N typically 4 to 6 W is “beam handling.
UBW2012, Berlin, December 2012 Jefferson Lab Experience with Beam Halo, Beam Loss and Related beam diagnostics Pavel Evtushenko, Steve Benson, Dave Douglas,
Gamma Beam Systems a simple introduction. Purpose of the machine Deliver a high performance photon beam: Variable energy Highly polarized High intensity.
Slide 1 George R. Neil Associate Director Jefferson Lab Jefferson Avenue Newport News, Virginia VUV Program Directors Review Plans for a VUV.
Thomas Roser RHIC Open Planning Meeting December 3-4, 2003 RHIC II machine plans Electron cooling at RHIC Luminosity upgrade parameters.
Generation and Characterization of Magnetized Bunched Electron Beam from DC Photogun for MEIC Cooler Laboratory Directed Research and Development (LDRD)
FEL Beam Dynami cs FEL Beam Dynamics T. Limberg FEL driver linac operation with very short electron bunches.
News from HZB / BESSY Wolfgang Anders at ESLS-RF Meeting September 2010 Trieste.
Injector Setup/Mini-phase  Description of injector setup  sources of drift  Mini-phase procedure for injector  Checking the rest of the machine. Stephen.
1 Energy recovery linacs Sverker Werin MAX-lab 8 July 2003.
1 Low-energy RHIC electron Cooler (LEReC) cost estimate December 2, 2014.
Accelerator and Detector R&D, August Diagnostics Related to the Unwanted Beam Pavel Evtushenko, Jlab FEL.
Low Emittance RF Gun Developments for PAL-XFEL
Compton polarimetry for EIC Jefferson Lab Compton Polarimeters.
FLASH Operation at DESY From a Test Accelerator to a User Facility Michael Bieler FLASH Operation at DESY WAO2012, SLAC, Aug. 8, 2012.
BERLinPro An ERL Demonstration facility at the HELMHOLTZ ZENTRUM BERLIN.
Machine Protection at the 1MW CEBAF Electron Accelerator and Free Electron Laser Facility Kelly Mahoney Presented at the Workshop for.
ERHIC design status V.Ptitsyn for the eRHIC design team.
Accelerator Science and Technology Centre Extended ALICE Injector J.W. McKenzie, B.D. Muratori, Y.M. Saveliev STFC Daresbury Laboratory,
14th ESLS RF Workshop ELETTRA / Trieste, Italy / 2010 September The Elettra Storage Ring and Top-Up Operation Emanuel Karantzoulis.
Thomas Roser EIC AC meeting November 3-4, 2009 EIC Accelerator R&D Strategy and Programs Thomas Roser/Andrew Hutton BNL / Jefferson Lab R&D program is.
1 ALICE and EMMA Yuri Saveliev … and many others at DL and beyond ASTeC, STFC Daresbury Laboratory IOP Particle Accelerators and Beams Annual Conference.
Electron Sources for ERLs – Requirements and First Ideas Andrew Burrill FLS 2012 “The workshop is intended to discuss technologies appropriate for a next.
Christopher Gerth DL/RAL Joint Workshop 28-29/4/04 Modelling of the ERLP injector system Christopher Gerth ASTeC, Daresbury Laboratory.
The Next Generation Light Source Test Facility at Daresbury Jim Clarke ASTeC, STFC Daresbury Laboratory Ultra Bright Electron Sources Workshop, Daresbury,
ERL Status and Plans at Jefferson Lab Stephen V. Benson, On behalf of the Jefferson Lab FEL team Current status Next Generation Soft X-ray Sources JLab.
MeRHIC Internal Cost Review October, Dmitry Kayran for injector group MeRHIC Internal Cost Review October 7-8, 2009 MeRHIC: Injection System Gun.
Future Circular Collider Study Kickoff Meeting CERN ERL TEST FACILITY STAGES AND OPTICS 12–15 February 2014, University of Geneva Alessandra Valloni.
J. Corlett. June 16, 2006 A Future Light Source for LBNL Facility Vision and R&D plan John Corlett ALS Scientific Advisory Committee Meeting June 16, 2006.
T. Atkinson*, A. Matveenko, A. Bondarenko, Y. Petenev Helmholtz-Zentrum Berlin für Materialien und Energie The Femto-Science Factory: A Multi-turn ERL.
Experience with Novosibirsk FEL Getmanov Yaroslav Budker INP, Russia Dec. 2012, Berlin, Germany Unwanted Beam Workshop.
PAL-XFEL Commissioning Plan ver. 1.1, August 2015 PAL-XFEL Beam Dynamics Group.
UBW2012, A. Matveenko Michael Abo-Bakr (presented by Alexander Matveenko) Unwanted Beam Workshop (UBW 2012) Dark Current Issues for Energy.
ESLS Workshop Nov 2015 MAX IV 3 GeV Ring Commissioning Pedro F. Tavares & Åke Andersson, on behalf of the whole MAX IV team.
Svb[General files ‘01/Presentations]PAC 10 kW laser input.ppt Operated by the Southeastern Universities Research Association for the U.S. Dept. of Energy.
WG2: Beam Dynamics, Optics and Instrumentation – Summary
An Electron source for PERLE
Beam Commissioning Adam Bartnik.
Novosibirsk ERL facility G.N. Kulipanov and NovoFEL team
Multi-bunch Operation for LCLS, LCLS_II, LCLS_2025
Beam dynamics for an X-band LINAC driving a 1 keV FEL
Plans of XFELO in Future ERL Facilities
Overview of LERF Status, Plans and Goals
Accelerators in a new light
R&D Topics for FOA Funding Proposals
Tunable Electron Bunch Train Generation at Tsinghua University
Joint Accelerator Research JGU & HZB
Dark current and halo tracking in ERLs
The Cornell High Brightness Injector
Machine Operation and Progresses in SSRF
ERL Main-Linac Cryomodule
ERL accelerator review. Parameters for a Compton source
VUV/Soft X-ray Oscillators
ERL EIC Workshop | Jefferson Laboratory | November 2, 2018
CLIC Feasibility Demonstration at CTF3
DC Photocathode Gun (JLAB)
小型X線源の性能確認実験計画 高輝度・RF電子銃研究会 広島大学 高エネルギー加速器研究機構 浦川順治
Andrew Hutton Concept suggested independently by Haipeng Wang
JLEIC Main Parameters with Strong Electron Cooling
Generation of Magnetized Bunched Electron Beam for MEIC Cooler
Presentation transcript:

Seesion1 summary Unwanted Beam Workshop (UBW 2012) Dark Current Issues for Energy Recovery Linacs

2 BERLinPro: Berlin Energy Recovery Project funding decision late 2010, start of project 2011 extensive gun development: Gun0.1 (2011), Gun0.2 (2012) and Gunlab 2015: first electrons from Gun2 & Booster  6 MeV 2017: merger 2018: 50 MeV recirculation

MEASURES AT DESIGN STAGE TO MINIMIZE EFFECT OF DARK BERLINPRO 3 Do not plan to operate at ultimate gradients Collimation is an issue Protect potentially weak places (water cooling of vacuum chambers) Diagnostics to control the unwanted beam losses Do the modeling … but do not believe it…

JLab IR/UV Upgrade E beam 135 MeV Bunch charge:60 pC – UV FEL 135 pC – IR FEL Rep. rate up to MHz 25 μJ/pulse in 250–700 nm UV-VIS 120 μJ/pulse in 1-10 μm IR

Conclusion / Summary  JLab FEL (IR/UV Upgrade)  RF gradients in LINAC always require attention, set radiation background level (FE)  HV-DC gun very tricky to process (new gun should improve it a lot) “Catch-22”  Drive Laser transport if made very carefully, seems to be not a problem  Drive Laser rep. rate control (EO cells) always need attention (extinction ration drifts)  Cathode suffers when conditioning and from breakdowns, still makes beam as needed, but scatters DL light – generates some halo  Non-linear beam dynamics is responsible for some fraction of the halo. When setting up for high current operation, a lot of effort and time goes in to “fitting” the halo through the recirculator, such that peak beam brightness does not suffer.  Radiation monitors, BLMs and vacuum are used as tuning diagnostics  CEBAF  NP detectors (background) require essentially no beam halo  Large statistics of cavity performance and its evolution (FE)  Direct effects of FE – RF trip rate, reduction of max. possible energy  Vacuum events related to beam loss (both high and very low current)

Lasing (1) Lasing (4) Lasing (2) groups of undulators and IR FELs (under construction and fabrication) One track in vertical plane (terahertz FEL) Common for all FELs accelerator system 6 Two tracks in a horizontal plane (IR FEL) Four tracks in a horizontal plane Full scale Novosibirsk FEL 6

Conclusion Unwanted beam losses can exist due to low-energy effects, lasing, and insufficiently flexibility of system in multipass mode. Protection system is working well in regular mode, should be changed for tuning and adjusting mode. Present status: at this time, in Novosibirsk FEL based on one-turn ERL operates with the highest power in terahertz region; FEL, based on the first in the world two-passes ERL, operates in infrared region; 95% energy recovery efficiency and 1 mA current are achieved at the four- pass ERL. 7